TWI806378B - Optical imaging lens - Google Patents
Optical imaging lens Download PDFInfo
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- TWI806378B TWI806378B TW111102917A TW111102917A TWI806378B TW I806378 B TWI806378 B TW I806378B TW 111102917 A TW111102917 A TW 111102917A TW 111102917 A TW111102917 A TW 111102917A TW I806378 B TWI806378 B TW I806378B
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B9/00—Optical objectives characterised both by the number of the components and their arrangements according to their sign, i.e. + or -
- G02B9/64—Optical objectives characterised both by the number of the components and their arrangements according to their sign, i.e. + or - having more than six components
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/001—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
- G02B13/0015—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design
- G02B13/002—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface
- G02B13/0045—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface having five or more lenses
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B1/00—Optical elements characterised by the material of which they are made; Optical coatings for optical elements
- G02B1/04—Optical elements characterised by the material of which they are made; Optical coatings for optical elements made of organic materials, e.g. plastics
- G02B1/041—Lenses
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/18—Optical objectives specially designed for the purposes specified below with lenses having one or more non-spherical faces, e.g. for reducing geometrical aberration
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B30/00—Camera modules comprising integrated lens units and imaging units, specially adapted for being embedded in other devices, e.g. mobile phones or vehicles
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- Optics & Photonics (AREA)
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Abstract
Description
本發明大致上關於一種光學成像鏡頭。具體而言,本發明特別是針對一種主要用於拍攝影像及錄影,並可以應用於可攜式電子產品之裝置,例如可應用於手機、相機、平板電腦、個人數位助理(Personal Digital Assistant,PDA)或頭戴裝置(AR、VR、MR)等電子裝置中的光學成像鏡頭。 The present invention generally relates to an optical imaging lens. Specifically, the present invention is particularly directed at a device mainly used for taking images and recording videos, and can be applied to portable electronic products, such as mobile phones, cameras, tablet computers, personal digital assistants (Personal Digital Assistant, PDA) ) or optical imaging lenses in electronic devices such as head-mounted devices (AR, VR, MR).
可攜式電子裝置的規格日新月異,其關鍵零組件-光學成像鏡頭也更加多樣化發展。對於可攜式電子裝置的主鏡頭不僅要求更大光圈並維持較短的系統長度外,還追求更高畫素與更高解析度。而高畫素隱含著必須增加鏡頭的像高,藉著採用更大的影像感測器來接受成像光線以提高畫素需求。但大光圈的設計使得鏡頭能接受更多的成像光線,使得設計的難度增加;而高畫素又使得鏡頭的解析度要提高,配合大光圈設計使得設計難度倍增。因此如何使鏡頭在有限的系統長度中加入多片透鏡,又要增加解析度且同時增大光圈與像高是需要挑戰並解決的問題。 The specifications of portable electronic devices are changing with each passing day, and their key components - optical imaging lenses are also becoming more diversified. The main lens of a portable electronic device not only requires a larger aperture and a shorter system length, but also pursues higher pixels and higher resolution. The high pixel size implies that the image height of the lens must be increased, and the pixel requirement is increased by using a larger image sensor to receive imaging light. However, the large aperture design allows the lens to accept more imaging light, making the design more difficult; while the high resolution increases the resolution of the lens, and the large aperture design makes the design more difficult. Therefore, how to add multiple lenses into the limited system length of the lens, increase the resolution and increase the aperture and image height at the same time is a problem that needs to be challenged and solved.
於是,本發明的各實施例提出一種具有較大光圈、較大像高與高解析度的八片式光學成像鏡頭。 Therefore, various embodiments of the present invention provide an eight-piece optical imaging lens with larger aperture, larger image height, and high resolution.
在本發明的一實施例中,第一透鏡具有正屈光率,且第一透鏡的像側面的圓周區域為凹面,第三透鏡的物側面的圓周區域為凹面,第六透鏡的像側面的光軸區域為凸面,第八透鏡的物側面的光軸區域為凸面,且第八透鏡的像側面的圓周區域為凸面,其中,光學成像鏡頭的透鏡只有上述八片,且滿足D41t51/(T3+G34)≧1.700的條件。 In one embodiment of the present invention, the first lens has a positive refractive power, and the circumferential area of the image side of the first lens is concave, the circumferential area of the object side of the third lens is concave, and the image side of the sixth lens is concave. The optical axis area is a convex surface, the optical axis area of the object side of the eighth lens is a convex surface, and the peripheral area of the image side of the eighth lens is a convex surface, wherein the optical imaging lens has only the above eight lenses, and satisfies D41t51/(T3 +G34)≧1.700 condition.
在本發明的另一實施例中,第三透鏡的物側面的圓周區域為凹面,第四透鏡的物側面的圓周區域為凹面,第六透鏡的像側面的光軸區域為凸面,第八透鏡的物側面的光軸區域為凸面,且第八透鏡的像側面的圓周區域為凸面,其中,光學成像鏡頭的透鏡只有上述八片,且滿足D41t51/(T3+G34)≧1.700的條件。 In another embodiment of the present invention, the peripheral region of the object side of the third lens is a concave surface, the peripheral region of the object side of the fourth lens is a concave surface, the optical axis region of the image side of the sixth lens is a convex surface, and the eighth lens The optical axis area on the object side is convex, and the circumference area on the image side of the eighth lens is convex, wherein the optical imaging lens has only the above eight lenses, and satisfies the condition of D41t51/(T3+G34)≧1.700.
在本發明的另一實施例中,第一透鏡具有正屈光率,且第一透鏡的像側面的圓周區域為凹面,第二透鏡具有負屈光率,第四透鏡的像側面的圓周區域為凸面,第六透鏡的像側面的光軸區域為凸面,第八透鏡的物側面的光軸區域為凸面,且第八透鏡的像側面的圓周區域為凸面,其中,光學成像鏡頭的透鏡只有上述八片,且滿足D41t61/(T3+G34)≧3.700的條件。 In another embodiment of the present invention, the first lens has positive refractive power, and the peripheral area of the image side of the first lens is concave, the second lens has negative refractive power, and the peripheral area of the image side of the fourth lens is is a convex surface, the optical axis area of the image side of the sixth lens is a convex surface, the optical axis area of the object side of the eighth lens is a convex surface, and the circumference area of the image side of the eighth lens is a convex surface, wherein the lens of the optical imaging lens has only The above eight pieces, and satisfy the condition of D41t61/(T3+G34)≧3.700.
在本發明的光學成像鏡頭中,實施例還可以進一步選擇性地滿足以下條件:D11t41/T4≦4.300;(D42t52+D62t82)/(G56+T6)≦4.100;EFL/(T1+T6+T8)≦4.000; TTL/(T1+G56+T6+T8)≦4.000;Fno*(T1+G12+T3+G34)/(T2+G23)≦3.110;3.800≦(ImgH+EPD+G56+T6)/D31t52;V3+V8≦100.000;V7+V8≦100.000;Fno*(T2+G34+T4+D62t82)/AAG≦3.600;6.100≦(ImgH+D41t62)/(G67+T7+G78);Fno*(ALT+BFL)/D41t62≦4.000;3.600≦EPD/(G67+T7);55.000≦V2+V6;Fno*TTL/EPD≦4.100;D31t42/T8≦2.700;(D11t41+D41t62)/D62t82≦5.400;以及3.000≦(EPD+EFL)/D11t41。 In the optical imaging lens of the present invention, embodiments can further selectively satisfy the following conditions: D11t41/T4≦4.300; (D42t52+D62t82)/(G56+T6)≦4.100; EFL/(T1+T6+T8) ≦4.000; TTL/(T1+G56+T6+T8)≦4.000; Fno*(T1+G12+T3+G34)/(T2+G23)≦3.110; 3.800≦(ImgH+EPD+G56+T6)/D31t52; V3+ V8≦100.000; V7+V8≦100.000; Fno*(T2+G34+T4+D62t82)/AAG≦3.600; 6.100≦(ImgH+D41t62)/(G67+T7+G78); Fno*(ALT+BFL)/ D41t62≦4.000; 3.600≦EPD/(G67+T7); 55.000≦V2+V6; Fno*TTL/EPD≦4.100; D31t42/T8≦2.700; EFL)/D11t41.
其中,T1定義為第一透鏡在光軸上的厚度;T2定義為第二透鏡在光軸上的厚度;T3定義為第三透鏡在光軸上的厚度;T4定義為第四透鏡在光軸上的厚度;T6定義為第六透鏡在光軸上的厚度;T7定義為第七透鏡在光軸上的厚度;T8定義為第八透鏡在光軸上的厚度;G12定義為第一透鏡到第二透鏡在光軸上的空氣間隙;G23定義為第二透鏡到第三透鏡在光軸上的空氣間隙;G34定義為第三透鏡到第四透鏡在光軸上的空氣間隙;G56定義為第五透鏡到第六透鏡在光軸上的空氣間隙;G67定義為第六透鏡到第七透鏡在光軸上的空氣間隙;G78定義為第七透鏡到第八透鏡在光軸上的空氣間隙;ALT定義為第一透鏡到第八透鏡在光軸上的八個透鏡之厚度總和;TTL定義為第一透鏡的物側面到成像面在 光軸上的距離;BFL定義為第八透鏡的像側面至成像面在光軸上的距離;AAG定義為第一透鏡到第八透鏡在光軸上的七個空氣間隙總和;EFL定義為光學成像鏡頭的有效焦距;ImgH定義為光學成像鏡頭的像高,Fno定義為光學成像鏡頭的光圈值,EPD定義為光學成像鏡頭的入瞳直徑,V2為第二透鏡的阿貝數;V3為第三透鏡的阿貝數;V6為第六透鏡的阿貝數;V7為第七透鏡的阿貝數;V8為第八透鏡的阿貝數。 Among them, T1 is defined as the thickness of the first lens on the optical axis; T2 is defined as the thickness of the second lens on the optical axis; T3 is defined as the thickness of the third lens on the optical axis; T4 is defined as the thickness of the fourth lens on the optical axis T6 is defined as the thickness of the sixth lens on the optical axis; T7 is defined as the thickness of the seventh lens on the optical axis; T8 is defined as the thickness of the eighth lens on the optical axis; G12 is defined as the thickness of the first lens to the The air gap of the second lens on the optical axis; G23 is defined as the air gap from the second lens to the third lens on the optical axis; G34 is defined as the air gap from the third lens to the fourth lens on the optical axis; G56 is defined as The air gap on the optical axis from the fifth lens to the sixth lens; G67 is defined as the air gap on the optical axis from the sixth lens to the seventh lens; G78 is defined as the air gap on the optical axis from the seventh lens to the eighth lens ; ALT is defined as the sum of the thicknesses of the eight lenses on the optical axis from the first lens to the eighth lens; TTL is defined as the distance from the object side to the imaging surface of the first lens The distance on the optical axis; BFL is defined as the distance from the image side of the eighth lens to the imaging surface on the optical axis; AAG is defined as the sum of the seven air gaps from the first lens to the eighth lens on the optical axis; EFL is defined as the optical The effective focal length of the imaging lens; ImgH is defined as the image height of the optical imaging lens, Fno is defined as the aperture value of the optical imaging lens, EPD is defined as the entrance pupil diameter of the optical imaging lens, V2 is the Abbe number of the second lens; V3 is the second The Abbe number of the three lenses; V6 is the Abbe number of the sixth lens; V7 is the Abbe number of the seventh lens; V8 is the Abbe number of the eighth lens.
另外,D41t51定義為第四透鏡的物側面到第五透鏡的物側面在光軸上的距離,D41t61定義為第四透鏡的物側面到第六透鏡的物側面在光軸上的距離,D11t41定義為第一透鏡的物側面到第四透鏡的物側面在光軸上的距離,D42t52定義為第四透鏡的像側面到第五透鏡的像側面在光軸上的距離,D62t82定義為第六透鏡的像側面到第八透鏡的像側面在光軸上的距離,D31t52為第三透鏡的物側面到第五透鏡的像側面在光軸上的距離,D41t62定義為第四透鏡的物側面到第六透鏡的像側面在光軸上的距離,D31t42定義為第三透鏡的物側面到第四透鏡的像側面在光軸上的距離。 In addition, D41t51 is defined as the distance on the optical axis from the object side of the fourth lens to the object side of the fifth lens on the optical axis, D41t61 is defined as the distance on the optical axis from the object side of the fourth lens to the object side of the sixth lens, and D11t41 defines is the distance on the optical axis from the object side of the first lens to the object side of the fourth lens on the optical axis, D42t52 is defined as the distance on the optical axis from the image side of the fourth lens to the image side of the fifth lens, and D62t82 is defined as the sixth lens D31t52 is the distance from the object side of the third lens to the image side of the fifth lens on the optical axis, D41t62 is defined as the object side of the fourth lens to the first lens The distance between the image side of the six lenses on the optical axis, D31t42 is defined as the distance from the object side of the third lens to the image side of the fourth lens on the optical axis.
1:光學成像鏡頭 1: Optical imaging lens
2:光圈 2: Aperture
3:濾光片 3: Filter
4:成像面 4: Imaging surface
11、21、31、41、51、61、71、81、110、410、510:物側面 11, 21, 31, 41, 51, 61, 71, 81, 110, 410, 510: the side of the object
12、22、32、42、52、62、72、82、120、320:像側面 12, 22, 32, 42, 52, 62, 72, 82, 120, 320: Like the side
13、16、23、26、33、36、43、46、53、56、63、66、73、76、83、86、Z1:光 軸區域 13, 16, 23, 26, 33, 36, 43, 46, 53, 56, 63, 66, 73, 76, 83, 86, Z1: light axis area
14、17、24、27、34、37、44、47、54、57、64、67、74、77、84、87、Z2:圓周區域 14, 17, 24, 27, 34, 37, 44, 47, 54, 57, 64, 67, 74, 77, 84, 87, Z2: Circumferential area
10:第一透鏡 10: First lens
20:第二透鏡 20: second lens
30:第三透鏡 30: Third lens
40:第四透鏡 40: Fourth lens
50:第五透鏡 50: fifth lens
60:第六透鏡 60: sixth lens
70:第七透鏡 70: seventh lens
80:第八透鏡 80: eighth lens
100、200、300、400、500:透鏡 100, 200, 300, 400, 500: lens
130:組裝部 130: Assembly Department
211、212:平行光線 211, 212: Parallel rays
A1:物側 A1: Object side
A2:像側 A2: image side
CP:中心點 CP: center point
CP1:第一中心點 CP1: first center point
CP2:第二中心點 CP2: second center point
TP1:第一轉換點 TP1: first transition point
TP2:第二轉換點 TP2: Second transition point
OB:光學邊界 OB: Optical Boundary
I:光軸 I: optical axis
Lc:主光線 Lc: chief light
Lm:邊緣光線 Lm: edge light
EL:延伸線 EL: extension line
Z3:中繼區域 Z3: relay zone
M:相交點 M: intersection point
R:相交點 R: intersection point
圖1至圖5繪示本發明光學成像鏡頭判斷曲率形狀方法之示意圖。 1 to 5 are schematic diagrams of the method for judging the curvature shape of the optical imaging lens of the present invention.
圖6繪示本發明光學成像鏡頭的第一實施例之示意圖。 FIG. 6 is a schematic diagram of the first embodiment of the optical imaging lens of the present invention.
圖7A繪示第一實施例在成像面上的縱向球差。 FIG. 7A shows the longitudinal spherical aberration on the imaging plane of the first embodiment.
圖7B繪示第一實施例在弧矢方向的場曲像差。 FIG. 7B shows the field curvature aberration in the sagittal direction of the first embodiment.
圖7C繪示第一實施例在子午方向的場曲像差。 FIG. 7C shows the field curvature aberration in the meridional direction of the first embodiment.
圖7D繪示第一實施例的畸變像差。 FIG. 7D illustrates the distortion aberration of the first embodiment.
圖8繪示本發明光學成像鏡頭的第二實施例之示意圖。 FIG. 8 is a schematic diagram of a second embodiment of the optical imaging lens of the present invention.
圖9A繪示第二實施例在成像面上的縱向球差。 FIG. 9A shows the longitudinal spherical aberration on the imaging plane of the second embodiment.
圖9B繪示第二實施例在弧矢方向的場曲像差。 FIG. 9B shows the field curvature aberration in the sagittal direction of the second embodiment.
圖9C繪示第二實施例在子午方向的場曲像差。 FIG. 9C shows the field curvature aberration in the meridional direction of the second embodiment.
圖9D繪示第二實施例的畸變像差。 FIG. 9D illustrates the distortion aberration of the second embodiment.
圖10繪示本發明光學成像鏡頭的第三實施例之示意圖。 FIG. 10 is a schematic diagram of a third embodiment of the optical imaging lens of the present invention.
圖11A繪示第三實施例在成像面上的縱向球差。 FIG. 11A shows the longitudinal spherical aberration on the imaging plane of the third embodiment.
圖11B繪示第三實施例在弧矢方向的場曲像差。 FIG. 11B shows the field curvature aberration in the sagittal direction of the third embodiment.
圖11C繪示第三實施例在子午方向的場曲像差。 FIG. 11C shows the field curvature aberration in the meridional direction of the third embodiment.
圖11D繪示第三實施例的畸變像差。 FIG. 11D shows the distortion aberration of the third embodiment.
圖12繪示本發明光學成像鏡頭的第四實施例之示意圖。 FIG. 12 is a schematic diagram of a fourth embodiment of the optical imaging lens of the present invention.
圖13A繪示第四實施例在成像面上的縱向球差。 FIG. 13A shows the longitudinal spherical aberration on the imaging plane of the fourth embodiment.
圖13B繪示第四實施例在弧矢方向的場曲像差。 FIG. 13B shows the field curvature aberration in the sagittal direction of the fourth embodiment.
圖13C繪示第四實施例在子午方向的場曲像差。 FIG. 13C shows the field curvature aberration in the meridian direction of the fourth embodiment.
圖13D繪示第四實施例的畸變像差。 FIG. 13D shows the distortion aberration of the fourth embodiment.
圖14繪示本發明光學成像鏡頭的第五實施例之示意圖。 FIG. 14 is a schematic diagram of a fifth embodiment of the optical imaging lens of the present invention.
圖15A繪示第五實施例在成像面上的縱向球差。 FIG. 15A shows the longitudinal spherical aberration on the imaging plane of the fifth embodiment.
圖15B繪示第五實施例在弧矢方向的場曲像差。 FIG. 15B shows the field curvature aberration in the sagittal direction of the fifth embodiment.
圖15C繪示第五實施例在子午方向的場曲像差。 FIG. 15C shows the field curvature aberration in the meridional direction of the fifth embodiment.
圖15D繪示第五實施例的畸變像差。 FIG. 15D shows the distortion aberration of the fifth embodiment.
圖16繪示本發明光學成像鏡頭的第六實施例之示意圖。 FIG. 16 is a schematic diagram of a sixth embodiment of the optical imaging lens of the present invention.
圖17A繪示第六實施例在成像面上的縱向球差。 FIG. 17A shows the longitudinal spherical aberration on the imaging plane of the sixth embodiment.
圖17B繪示第六實施例在弧矢方向的場曲像差。 FIG. 17B shows the field curvature aberration in the sagittal direction of the sixth embodiment.
圖17C繪示第六實施例在子午方向的場曲像差。 FIG. 17C shows the field curvature aberration in the meridional direction of the sixth embodiment.
圖17D繪示第六實施例的畸變像差。 FIG. 17D shows the distortion aberration of the sixth embodiment.
圖18繪示本發明光學成像鏡頭的第七實施例之示意圖。 FIG. 18 is a schematic diagram of a seventh embodiment of the optical imaging lens of the present invention.
圖19A繪示第七實施例在成像面上的縱向球差。 FIG. 19A shows the longitudinal spherical aberration on the imaging plane of the seventh embodiment.
圖19B繪示第七實施例在弧矢方向的場曲像差。 FIG. 19B shows the field curvature aberration in the sagittal direction of the seventh embodiment.
圖19C繪示第七實施例在子午方向的場曲像差。 FIG. 19C shows the field curvature aberration in the meridional direction of the seventh embodiment.
圖19D繪示第七實施例的畸變像差。 FIG. 19D shows the distortion aberration of the seventh embodiment.
圖20表示第一實施例詳細的光學數據。 Fig. 20 shows detailed optical data of the first embodiment.
圖21表示第一實施例詳細的非球面數據。 Fig. 21 shows detailed aspheric data of the first embodiment.
圖22表示第二實施例詳細的光學數據。 Fig. 22 shows detailed optical data of the second embodiment.
圖23表示第二實施例詳細的非球面數據。 Fig. 23 shows detailed aspheric data of the second embodiment.
圖24表示第三實施例詳細的光學數據。 Fig. 24 shows detailed optical data of the third embodiment.
圖25表示第三實施例詳細的非球面數據。 Fig. 25 shows detailed aspheric data of the third embodiment.
圖26表示第四實施例詳細的光學數據。 Fig. 26 shows detailed optical data of the fourth embodiment.
圖27表示第四實施例詳細的非球面數據。 Fig. 27 shows detailed aspheric data of the fourth embodiment.
圖28表示第五實施例詳細的光學數據。 Fig. 28 shows detailed optical data of the fifth embodiment.
圖29表示第五實施例詳細的非球面數據。 Fig. 29 shows detailed aspheric data of the fifth embodiment.
圖30表示第六實施例詳細的光學數據。 Fig. 30 shows detailed optical data of the sixth embodiment.
圖31表示第六實施例詳細的非球面數據。 Fig. 31 shows detailed aspheric data of the sixth embodiment.
圖32表示第七實施例詳細的光學數據。 Fig. 32 shows detailed optical data of the seventh embodiment.
圖33表示第七實施例詳細的非球面數據。 Fig. 33 shows detailed aspheric data of the seventh embodiment.
圖34表示各實施例之重要參數。 Figure 34 shows the important parameters of each embodiment.
圖35表示各實施例之重要參數。 Figure 35 shows the important parameters of each embodiment.
本說明書和申請專利範圍中使用的用語「光軸區域」、「圓周區域」、「凹面」和「凸面」應基於本說明書中列出的定義來解釋。 The terms "optical axis area", "circumferential area", "concave" and "convex" used in this specification and claims should be interpreted based on the definitions listed in this specification.
本說明書之光學系統包含至少一透鏡,接收入射光學系統之平行於光軸至相對光軸呈半視角(HFOV)角度內的成像光線。成像光線通過光學系統於成像面上成像。所言之「一透鏡具有正屈光率(或負屈光率)」,是指所述透鏡以高斯光學理論計算出來之近軸屈光率為正(或為負)。所言之「透鏡之物側面(或像側面)」定義為成像光線通過透鏡表面的特定範圍。成像光線包括至少兩類光線:主光線(chief ray)Lc及邊緣光線(marginal ray)Lm(如圖1所示)。透鏡之物側面(或像側面)可依不同位置區分為不同區域,包含光軸區域、圓周區域、或在部分實施例中的一個或多個中繼區域,該些區域的說明將於下方詳細闡述。 The optical system of the present specification includes at least one lens, which receives the imaging light from the incident optical system parallel to the optical axis to within an angle of half field of view (HFOV) relative to the optical axis. The imaging light is imaged on the imaging plane through the optical system. The term "a lens has a positive refractive power (or negative refractive power)" means that the paraxial refractive power of the lens calculated by Gaussian optical theory is positive (or negative). The so-called "object side (or image side) of the lens" is defined as a specific range where imaging light passes through the lens surface. The imaging light includes at least two types of light: chief ray Lc and marginal ray Lm (as shown in FIG. 1 ). The object side (or image side) of the lens can be divided into different areas according to different positions, including the optical axis area, the circumference area, or one or more relay areas in some embodiments, and the description of these areas will be described in detail below. elaborate.
圖1為透鏡100的徑向剖視圖。定義透鏡100表面上的二參考點:中心點及轉換點。透鏡表面的中心點為該表面與光軸I的一交點。如圖1所例示,第一中心點CP1位於透鏡100的物側面110,第二中心點CP2位於透鏡100的像側面120。轉換點是位於透鏡表面上的一點,且該點的切線與光軸I垂直。定義透鏡表面之光學邊界OB為通過該透鏡表面徑向最外側的邊緣光線Lm與該透鏡表面相交的一點。所有的轉換點皆位於光軸I與透鏡表面之光學邊界OB之間。除此之外,透鏡100表面可能不具有轉換點或具有至少一轉換點,若單一透鏡表面有複數個轉換點,則該些轉換點由徑向向外的方向依序自第一轉換點開始命名。例如,第一轉換點TP1(最靠近光軸I)、第二轉換點TP2(如圖4所示)及第N轉換點(距離光軸I最遠)。
FIG. 1 is a radial cross-sectional view of a
當透鏡表面具有至少一轉換點,定義從中心點至第一轉換點TP1的範圍為光軸區域,其中,該光軸區域包含中心點。定義距離光軸I最遠的轉換點(第N轉換點)徑向向外至光學邊界OB的區域為圓周區域。在部分實施例中,可另包含介於光軸區域與圓周區域之間的中繼區域,中繼區域的數量取決於轉換點的數量。當透鏡表面不具有轉換點,定義自光軸I起算至透鏡表面光學邊界OB之間距離的0%~50%為光軸區域,自光軸I起算至透鏡表面光學邊界OB之間距離的50%~100%為圓周區域。 When the lens surface has at least one transition point, the range from the central point to the first transition point TP1 is defined as the optical axis area, wherein the optical axis area includes the central point. Define the area from the conversion point farthest from the optical axis I (the Nth conversion point) radially outward to the optical boundary OB as the circumferential area. In some embodiments, a relay area between the optical axis area and the circumference area may be further included, and the number of the relay area depends on the number of conversion points. When there is no conversion point on the lens surface, define 0%~50% of the distance from the optical axis I to the optical boundary OB of the lens surface as the optical axis area, and 50% of the distance from the optical axis I to the optical boundary OB of the lens surface %~100% is the circumference area.
當平行光軸I之光線通過一區域後,若光線朝光軸I偏折且與光軸I的交點位在透鏡像側A2,則該區域為凸面。當平行光軸I之光線通過一區域後,若光線的延伸線與光軸I的交點位在透鏡物側A1,則該區域為凹面。 When the light parallel to the optical axis I passes through a region, if the light is deflected toward the optical axis I and the intersection with the optical axis I is on the image side A2 of the lens, then the region is a convex surface. After the light rays parallel to the optical axis I pass through a region, if the intersection of the extension line of the light rays and the optical axis I is on the object side A1 of the lens, the region is a concave surface.
除此之外,參見圖1,透鏡100還可包含一由光學邊界OB徑向向外延伸的組裝部130。組裝部130一般來說用以供該透鏡100組裝於光學系統之一相對應元件(圖未示)。成像光線並不會到達該組裝部130。組裝部130之結構與形狀僅為說明本發明之示例,不以此限制本發明的範圍。下列討論之透鏡的組裝部130可能會在圖式中被部分或全部省略。
In addition, referring to FIG. 1 , the
參見圖2,定義中心點CP與第一轉換點TP1之間為光軸區域Z1。定義第一轉換點TP1與透鏡表面的光學邊界OB之間為圓周區域Z2。如圖2所示,平行光線211在通過光軸區域Z1後與光軸I在透鏡200的像側A2相交,即平行光線211通過光軸區域Z1的焦點位於透鏡200像側A2的R點。由於光線與光軸I相交於透鏡200像側A2,故光軸區域Z1為凸面。反之,平行光線212在通過圓周區域Z2後發散。如圖2所示,平行光線212通過圓周區域Z2後的延伸線EL與光軸I在透鏡200
的物側A1相交,即平行光線212通過圓周區域Z2的焦點位於透鏡200物側A1的M點。由於光線的延伸線EL與光軸I相交於透鏡200物側A1,故圓周區域Z2為凹面。於圖2所示的透鏡200中,第一轉換點TP1是光軸區域與圓周區域的分界,即第一轉換點TP1為凸面轉凹面的分界點。
Referring to FIG. 2 , the optical axis zone Z1 is defined between the central point CP and the first transition point TP1 . A circumferential zone Z2 is defined between the first transition point TP1 and the optical boundary OB of the lens surface. As shown in FIG. 2 , the
另一方面,光軸區域的面形凹凸判斷還可依該領域中通常知識者的判斷方式,即藉由近軸的曲率半徑(簡寫為R值)的正負號來判斷透鏡之光軸區域面形的凹凸。R值可常見被使用於光學設計軟體中,例如Zemax或CodeV。R值亦常見於光學設計軟體的透鏡資料表(lens data sheet)中。以物側面來說,當R值為正時,判定為物側面的光軸區域為凸面;當R值為負時,判定物側面的光軸區域為凹面。反之,以像側面來說,當R值為正時,判定像側面的光軸區域為凹面;當R值為負時,判定像側面的光軸區域為凸面。此方法判定的結果與前述藉由光線/光線延伸線與光軸的交點判定方式的結果一致,光線/光線延伸線與光軸交點的判定方式即為以一平行光軸之光線的焦點位於透鏡之物側或像側來判斷面形凹凸。本說明書所描述之「一區域為凸面(或凹面)」、「一區域為凸(或凹)」或「一凸面(或凹面)區域」可被替換使用。 On the other hand, the judgment of the concave-convex surface shape of the optical axis area can also be judged according to the judgment method of ordinary knowledge in this field, that is, the optical axis area surface of the lens can be judged by the sign of the paraxial curvature radius (abbreviated as R value). shaped bumps. R-values are commonly used in optical design software such as Zemax or CodeV. The R value is also commonly found in the lens data sheet of optical design software. For the object side, when the R value is positive, it is judged that the optical axis area on the object side is convex; when the R value is negative, it is judged that the optical axis area on the object side is concave. Conversely, for the image side, when the R value is positive, the optical axis area on the image side is judged to be concave; when the R value is negative, the optical axis area on the image side is judged to be convex. The judgment result of this method is consistent with the above-mentioned result of judging the intersection point of the ray/ray extension line and the optical axis. The judgment method of the intersection point of the ray/ray extension line and the optical axis is that the focal point of a ray parallel to the optical axis is located on the lens Use the object side or the image side to judge the unevenness of the surface. "A region is convex (or concave)", "a region is convex (or concave)" or "a convex (or concave) region" described in this specification can be used interchangeably.
圖3至圖5提供了在各個情況下判斷透鏡區域的面形及區域分界的範例,包含前述之光軸區域、圓周區域及中繼區域。 3 to 5 provide examples of judging the surface shape and area boundary of the lens area in each case, including the aforementioned optical axis area, circumference area, and relay area.
圖3為透鏡300的徑向剖視圖。參見圖3,透鏡300的像側面320在光學邊界OB內僅存在一個轉換點TP1。透鏡300的像側面320的光軸區域Z1及圓周區域Z2如圖3所示。此像側面320的R值為正(即R>0),因此,光軸區域Z1為凹面。
FIG. 3 is a radial cross-sectional view of the
一般來說,以轉換點為界的各個區域面形會與相鄰的區域面形相反,因此,可用轉換點來界定面形的轉變,即自轉換點由凹面轉凸面或由凸面轉凹面。於圖3中,由於光軸區域Z1為凹面,面形於轉換點TP1轉變,故圓周區域Z2為凸面。 Generally speaking, the surface shape of each area bounded by the conversion point will be opposite to that of the adjacent area. Therefore, the conversion point can be used to define the transformation of the surface shape, that is, from the conversion point to the concave surface to the convex surface or from the convex surface to the concave surface. In FIG. 3 , since the optical axis zone Z1 is a concave surface, and the surface shape changes at the transition point TP1 , the peripheral zone Z2 is a convex surface.
圖4為透鏡400的徑向剖視圖。參見圖4,透鏡400的物側面410存在一第一轉換點TP1及一第二轉換點TP2。定義光軸I與第一轉換點TP1之間為物側面410的光軸區域Z1。此物側面410的R值為正(即R>0),因此,光軸區域Z1為凸面。
FIG. 4 is a radial cross-sectional view of the
定義第二轉換點TP2與透鏡400的物側面410的光學邊界OB之間為圓周區域Z2,該物側面410的該圓周區域Z2亦為凸面。除此之外,定義第一轉換點TP1與第二轉換點TP2之間為中繼區域Z3,該物側面410的該中繼區域Z3為凹面。再次參見圖4,物側面410由光軸I徑向向外依序包含光軸I與第一轉換點TP1之間的光軸區域Z1、位於第一轉換點TP1與第二轉換點TP2之間的中繼區域Z3,及第二轉換點TP2與透鏡400的物側面410的光學邊界OB之間的圓周區域Z2。由於光軸區域Z1為凸面,面形自第一轉換點TP1轉變為凹,故中繼區域Z3為凹面,又面形自第二轉換點TP2再轉變為凸,故圓周區域Z2為凸面。
A circumferential area Z2 is defined between the second transition point TP2 and the optical boundary OB of the
圖5為透鏡500的徑向剖視圖。透鏡500的物側面510無轉換點。對於無轉換點的透鏡表面,例如透鏡500的物側面510,定義自光軸I起算至透鏡表面光學邊界OB之間距離的0%~50%為光軸區域,自光軸I起算至透鏡表面光學邊界OB之間距離的50%~100%為圓周區域。參見圖5所示之透鏡500,定義光軸I至自光軸I起算到透鏡500表面光學邊界OB之間距離的50%為物側面510的光軸區域
Z1。此物側面510的R值為正(即R>0),因此,光軸區域Z1為凸面。由於透鏡500的物側面510無轉換點,因此物側面510的圓周區域Z2亦為凸面。透鏡500更可具有組裝部(圖未示)自圓周區域Z2徑向向外延伸。
FIG. 5 is a radial cross-sectional view of the
如圖6所示,本發明光學成像鏡頭1,從放置物體(圖未示)的物側A1至成像的像側A2,沿著光軸(optical axis)I,主要由八片透鏡所構成,依序包含有第一透鏡10、第二透鏡20、第三透鏡30、第四透鏡40、第五透鏡50、第六透鏡60、第七透鏡70、第八透鏡80以及成像面(image plane)4。一般來說,第一透鏡10、第二透鏡20、第三透鏡30、第四透鏡40、第五透鏡50、第六透鏡60、第七透鏡70以及第八透鏡80都可以是由透明的塑膠材質所製成,但本發明不以此為限。在本發明光學成像鏡頭1中的透鏡總共只有第一透鏡10、第二透鏡20、第三透鏡30、第四透鏡40、第五透鏡50、第六透鏡60、第七透鏡70與第八透鏡80這八片透鏡。光軸I為整個光學成像鏡頭1的光軸,所以每片透鏡的光軸和光學成像鏡頭1的光軸都是相同的。
As shown in FIG. 6, the
此外,本光學成像鏡頭1還包含光圈(aperture stop)2,設置於適當之位置。在圖6中,光圈2是設置在第一透鏡10朝向物側A1的一側,換句話說,第一透鏡10是設置在光圈2與第二透鏡20之間。當由位於物側A1之待拍攝物(圖未示)所發出的光線(圖未示)進入本發明光學成像鏡頭1時,即會依序經由光圈2、第一透鏡10、第二透鏡20、第三透鏡30、第四透鏡40、第五透鏡50、第六透鏡60、第七透鏡70、第八透鏡80與濾光片3之後,光線會在像側A2的成像面4上聚焦而形成清晰的影像。在本發明各實施例中,濾光片3是設於第八透鏡80與成像面4之間,其可以是具有各種合適功能之濾鏡,例如:紅外線截止濾光片(IR cut filter),其用以避免成像光線中的紅外線傳遞至成像面4而影響成像品質。
In addition, the
本發明光學成像鏡頭1中之各個透鏡,都分別具有朝向物側A1且使成像光線通過的物側面,與朝向像側A2且使成像光線通過的像側面。另外,本發明光學成像鏡頭1中之各個透鏡,亦都分別具有光軸區域與圓周區域。例如,第一透鏡10具有物側面11與像側面12;第二透鏡20具有物側面21與像側面22;第三透鏡30具有物側面31與像側面32;第四透鏡40具有物側面41與像側面42;第五透鏡50具有物側面51與像側面52;第六透鏡60具有物側面61與像側面62;第七透鏡70具有物側面71與像側面72;第八透鏡80具有物側面81與像側面82。各物側面與像側面又分別有光軸區域以及圓周區域。
Each lens in the
本發明光學成像鏡頭1中之各個透鏡,還都分別具有位在光軸I上的厚度T。例如,第一透鏡10具有第一透鏡厚度T1、第二透鏡20具有第二透鏡厚度T2、第三透鏡30具有第三透鏡厚度T3、第四透鏡40具有第四透鏡厚度T4、第五透鏡50具有第五透鏡厚度T5、第六透鏡60具有第六透鏡厚度T6、第七透鏡70具有第七透鏡厚度T7、第八透鏡80具有第八透鏡厚度T8。所以,本發明的光學成像鏡頭1中從第一透鏡10到第八透鏡80在光軸I上的八個透鏡之厚度總和稱為ALT。也就是,ALT=T1+T2+T3+T4+T5+T6+T7+T8。
Each lens in the
另外,在本發明光學成像鏡頭1中,在各個透鏡之間又具有位在光軸I上的空氣間隙(air gap)。例如,第一透鏡10與第二透鏡20的空氣間隙稱為G12、第二透鏡20與第三透鏡30的空氣間隙稱為G23、第三透鏡30與第四透鏡40的空氣間隙稱為G34、第四透鏡40與第五透鏡50的空氣間隙稱為G45、第五透鏡50與第六透鏡60的空氣間隙稱為G56、第六透鏡60與第七透鏡70的空氣間隙稱為G67、第七透鏡70與第八透鏡80的空氣間隙稱為G78。所以,從第一透鏡10到第八透鏡
80在光軸I上的七個空氣間隙之總和即稱為AAG。亦即,AAG=G12+G23+G34+G45+G56+G67+G78。
In addition, in the
另外,第一透鏡10的物側面11至成像面4在光軸I上的距離,為光學成像鏡頭1的系統長度TTL。光學成像鏡頭1的有效焦距為EFL。第一透鏡10的物側面11至第八透鏡80的像側面82在光軸I上的距離為TL。HFOV為光學成像鏡頭1的半視角,即最大視角(Field of View)的一半。ImgH為光學成像鏡頭1的像高,Fno為光學成像鏡頭1的光圈值,EPD為光學成像鏡頭的入瞳直徑(Entrance Pupil Diameter),等於光學成像鏡頭1的有效焦距EFL除以光圈值Fno。
In addition, the distance on the optical axis I from the
當安排濾光片3介於第八透鏡80和成像面4之間時,G8F代表第八透鏡80與濾光片3在光軸I上的空氣間隙、TF代表濾光片3在光軸I上的厚度、GFP代表濾光片3與成像面4在光軸I上的空氣間隙、BFL為光學成像鏡頭1的後焦距,即第八透鏡80的像側面82到成像面4在光軸I上的距離,即BFL=G8F+TF+GFP。
When the
另外,再定義:f1為第一透鏡10的焦距;f2為第二透鏡20的焦距;f3為第三透鏡30的焦距;f4為第四透鏡40的焦距;f5為第五透鏡50的焦距;f6為第六透鏡60的焦距;f7為第七透鏡70的焦距;f8為第八透鏡80的焦距;n1為第一透鏡10的折射率;n2為第二透鏡20的折射率;n3為第三透鏡30的折射率;n4為第四透鏡40的折射率;n5為第五透鏡50的折射率;n6為第六透鏡60的折射率;n7為第七透鏡70的折射率;n8為第八透鏡80的折射率;V1為第一透鏡10的阿貝數;V2為第二透鏡20的阿貝數;V3為第三透鏡30的阿貝數;V4為第四透鏡40的阿貝數;V5為第五透鏡50的阿貝數;V6為第六透鏡60的阿貝數;V7為第七透鏡70的阿貝數;V8為第八透鏡80的阿貝數。 In addition, redefine: f1 is the focal length of the first lens 10; f2 is the focal length of the second lens 20; f3 is the focal length of the third lens 30; f4 is the focal length of the fourth lens 40; f5 is the focal length of the fifth lens 50; f6 is the focal length of the sixth lens 60; f7 is the focal length of the seventh lens 70; f8 is the focal length of the eighth lens 80; n1 is the refractive index of the first lens 10; n2 is the refractive index of the second lens 20; The refractive index of three lenses 30; n4 is the refractive index of the fourth lens 40; n5 is the refractive index of the fifth lens 50; n6 is the refractive index of the sixth lens 60; n7 is the refractive index of the seventh lens 70; The refractive index of eight lenses 80; V1 is the Abbe number of the first lens 10; V2 is the Abbe number of the second lens 20; V3 is the Abbe number of the third lens 30; V4 is the Abbe number of the fourth lens 40 V5 is the Abbe number of the fifth lens 50; V6 is the Abbe number of the sixth lens 60; V7 is the Abbe number of the seventh lens 70; V8 is the Abbe number of the eighth lens 80.
本發明中另外定義,D41t51為第四透鏡40的物側面41到第五透鏡50的物側面51在光軸I上的距離,D41t61為第四透鏡40的物側面41到第六透鏡60的物側面61在光軸I上的距離,D11t41為第一透鏡10的物側面11到第四透鏡40的物側面41在光軸I上的距離,D42t52為第四透鏡40的像側面42到第五透鏡50的像側面52在光軸I上的距離,D62t82為第六透鏡60的像側面62到第八透鏡80的像側面82在光軸I上的距離,D31t52為第三透鏡30的物側面31到第五透鏡50的像側面52在光軸I上的距離,D41t62為第四透鏡40的物側面41到第六透鏡60的像側面62在光軸I上的距離,D31t42為第三透鏡30的物側面31到第四透鏡40的像側面42在光軸I上的距離。
Additionally defined in the present invention, D41t51 is the distance on the optical axis I from the
第一實施例 first embodiment
請參閱圖6,例示本發明光學成像鏡頭1的第一實施例。第一實施例在成像面4上的縱向球差(longitudinal spherical aberration)請參考圖7A、弧矢(sagittal)方向的場曲(field curvature)像差請參考圖7B、子午(tangential)方向的場曲像差請參考圖7C、以及畸變像差(distortion aberration)請參考圖7D。所有實施例中各球差圖之Y軸代表視場,其最高點均為1.0,實施例中各像差圖及畸變像差圖之Y軸代表像高,第一實施例的像高(Image Height,ImgH)為5.467毫米。
Please refer to FIG. 6 , which illustrates the first embodiment of the
第一實施例之光學成像鏡頭1主要由八枚具有屈光率之透鏡、光圈2、與成像面4所構成。第一實施例之光圈2是設置在第一透鏡10朝向物側A1的一側。
The
第一透鏡10具有正屈光率,第一透鏡10的物側面11的光軸區域13為凸面以及其圓周區域14為凸面,第一透鏡10的像側面12的光軸區域16為凹面以及其圓周區域17為凹面。第一透鏡10之物側面11及像側面12均為非球面,但不以此為限。
The
第二透鏡20具有負屈光率,第二透鏡20的物側面21的光軸區域23為凸面以及其圓周區域24為凸面,第二透鏡20的像側面22的光軸區域26為凹面以及其圓周區域27為凹面。第二透鏡20之物側面21及像側面22均為非球面,但不以此為限。
The
第三透鏡30具有負屈光率,第三透鏡30的物側面31的光軸區域33為凹面以及其圓周區域34為凹面,第三透鏡30的像側面32的光軸區域36為凹面以及其圓周區域37為凸面。第三透鏡30之物側面31及像側面32均為非球面,但不以此為限。
The
第四透鏡40具有正屈光率,第四透鏡40的物側面41的光軸區域43為凹面以及其圓周區域44為凹面,第四透鏡40的像側面42的光軸區域46為凸面以及其圓周區域47為凸面。第四透鏡40之物側面41及像側面42均為非球面,但不以此為限。
The
第五透鏡50具有正屈光率,第五透鏡50的物側面51的光軸區域53為凸面以及其圓周區域54為凹面,第五透鏡50的像側面52的光軸區域56為凹面以及其圓周區域57為凸面。第五透鏡50之物側面51及像側面52均為非球面,但不以此為限。
The
第六透鏡60具有負屈光率,第六透鏡60的物側面61的光軸區域63為凹面以及其圓周區域64為凹面,第六透鏡60的像側面62的光軸區域66為凸面以及其圓周區域67為凸面。第六透鏡60之物側面61及像側面62均為非球面,但不以此為限。
The
第七透鏡70具有負屈光率,第七透鏡70的物側面71的光軸區域73為凸面以及其圓周區域74為凹面,第七透鏡70的像側面72的光軸區域76為凹面以及其圓周區域77為凸面。第七透鏡70之物側面71及像側面72均為非球面,但不以此為限。
The
第八透鏡80具有負屈光率,第八透鏡80的物側面81的光軸區域83為凸面以及其圓周區域84為凸面,第八透鏡80的像側面82的光軸區域86為凹面以及其圓周區域87為凸面。第八透鏡80之物側面81及像側面82均為非球面,但不以此為限。
The
在本發明光學成像鏡頭1中,從第一透鏡10到第八透鏡80中,所有的物側面11/21/31/41/51/61/71/81與像側面12/22/32/42/52/62/72/82共計十六個曲面均可以為非球面,但不以此為限。若為非球面,則此等非球面係經由下列公式所定義:
其中:Y表示非球面曲面上的點與光軸I的垂直距離; Z表示非球面之深度(非球面上距離光軸I為Y的點,其與相切於非球面光軸I上頂點之切面,兩者間的垂直距離);R表示透鏡表面近光軸I處之曲率半徑;K為圓錐係數(conic constant);ai為第i階非球面係數,其中各實施例的a2係數均為0。 Among them: Y represents the vertical distance between the point on the aspheric surface and the optical axis I; Z represents the depth of the aspheric surface (the point on the aspheric surface that is Y from the optical axis I is tangent to the vertex on the aspheric optical axis I tangential plane, the vertical distance between the two); R represents the radius of curvature at the near optical axis I of the lens surface; K is the conic coefficient ( conic constant); Both are 0.
第一實施例光學成像鏡頭系統的光學數據如圖20所示,非球面數據如圖21所示。值得注意的是,本實施例以及以下各實施例中,非球面數據的表格中a2欄位數值均為0,因此各實施例省略a2欄位。在以下實施例之光學成像鏡頭系統中,整體光學成像鏡頭的光圈值(f-number)為Fno、有效焦距為(EFL)、半視角(Half Field of View,簡稱HFOV)為整體光學成像鏡頭中最大視角(Field of View)的一半,其中,光學成像鏡頭的像高(ImgH)、曲率半徑、厚度及焦距的單位均為毫米(mm)。本實施例中,EFL=7.711毫米;HFOV=40.842度;TTL=9.798毫米;Fno=1.702;ImgH=5.467毫米。 The optical data of the optical imaging lens system of the first embodiment is shown in FIG. 20 , and the aspherical data is shown in FIG. 21 . It should be noted that, in this embodiment and the following embodiments, the value of column a2 in the aspherical data table is all 0, so the column a2 is omitted in each embodiment. In the optical imaging lens system of the following embodiments, the aperture value (f-number) of the overall optical imaging lens is Fno, the effective focal length is (EFL), and the half field of view (Half Field of View, referred to as HFOV) is in the overall optical imaging lens Half of the maximum field of view (Field of View), where the image height (ImgH), radius of curvature, thickness and focal length of the optical imaging lens are all in millimeters (mm). In this embodiment, EFL=7.711 mm; HFOV=40.842 degrees; TTL=9.798 mm; Fno=1.702; ImgH=5.467 mm.
第二實施例 second embodiment
請參閱圖8,例示本發明光學成像鏡頭1的第二實施例。請注意,從第二實施例開始,為簡化並清楚表達圖式,僅在圖上特別標示各透鏡與第一實施例不同面形的光軸區域與圓周區域,而其餘與第一實施例的透鏡相同的面形的光軸區域與圓周區域,例如凹面或是凸面則不另外標示。第二實施例在成像面4上的縱向球差請參考圖9A、弧矢方向的場曲像差請參考圖9B、子午方向的場曲像差請參考圖9C、畸變像差請參考圖9D。第二實施例之設計與第一實施例類似,不同之處在於,透鏡屈光率、透鏡曲率半徑、透鏡厚度、透鏡非球面係數或是後焦距等相關參數有別。此外,本實施例中,第三透鏡30的物側面31的光
軸區域33為凸面,第四透鏡40的物側面41的光軸區域43為凸面,第五透鏡50具有負屈光率,第六透鏡60具有正屈光率,第六透鏡60的物側面61的光軸區域63為凸面,第八透鏡80的物側面81的圓周區域84為凹面。
Please refer to FIG. 8 , which illustrates a second embodiment of the
第二實施例詳細的光學數據如圖22所示,非球面數據如圖23所示。本實施例中,EFL=8.398毫米;HFOV=40.842度;TTL=10.014毫米;Fno=1.854;ImgH=5.849毫米。特別是:1.本實施例鏡片光軸區域與圓周區域厚薄差異比第一實施例小,易於製造因此良率較高。 The detailed optical data of the second embodiment is shown in FIG. 22 , and the aspheric data is shown in FIG. 23 . In this embodiment, EFL=8.398 mm; HFOV=40.842 degrees; TTL=10.014 mm; Fno=1.854; ImgH=5.849 mm. In particular: 1. The thickness difference between the optical axis area and the peripheral area of the lens in this embodiment is smaller than that in the first embodiment, which is easy to manufacture and thus has a higher yield.
第三實施例 third embodiment
請參閱圖10,例示本發明光學成像鏡頭1的第三實施例。第三實施例在成像面4上的縱向球差請參考圖11A、弧矢方向的場曲像差請參考圖11B、子午方向的場曲像差請參考圖11C、畸變像差請參考圖11D。第三實施例之設計與第一實施例類似,不同之處在於,透鏡屈光率、透鏡曲率半徑、透鏡厚度、透鏡非球面係數或是後焦距等相關參數有別。
Please refer to FIG. 10 , which illustrates a third embodiment of the
第三實施例詳細的光學數據如圖24所示,非球面數據如圖25所示,本實施例中,EFL=8.647毫米;HFOV=40.842度;TTL=9.384毫米;Fno=1.909;ImgH=5.742毫米。特別是:1.本實施例的系統長度TTL比第一實施例的系統長度TTL短;2.本實施例的畸變像差優於第一實施例的畸變像差。 The detailed optical data of the third embodiment is shown in Figure 24, and the aspheric data is shown in Figure 25. In this embodiment, EFL=8.647 mm; HFOV=40.842 degrees; TTL=9.384 mm; Fno=1.909; ImgH=5.742 mm. In particular: 1. The system length TTL of this embodiment is shorter than that of the first embodiment; 2. The distortion aberration of this embodiment is better than that of the first embodiment.
第四實施例 Fourth embodiment
請參閱圖12,例示本發明光學成像鏡頭1的第四實施例。第四實施例在成像面4上的縱向球差請參考圖13A、弧矢方向的場曲像差請參考圖13B、子午
方向的場曲像差請參考圖13C、畸變像差請參考圖13D。第四實施例之設計與第一實施例類似,不同之處在於,透鏡屈光率、透鏡曲率半徑、透鏡厚度、透鏡非球面係數或是後焦距等相關參數有別。此外,本實施例中,第三透鏡30的物側面31的光軸區域33為凸面,第五透鏡50具有負屈光率,第六透鏡60具有正屈光率,第六透鏡60的物側面61的光軸區域63為凸面,第七透鏡70具有正屈光率,第八透鏡80的物側面81的圓周區域84為凹面。
Please refer to FIG. 12 , which illustrates a fourth embodiment of the
第四實施例詳細的光學數據如圖26所示,非球面數據如圖27所示。本實施例中,EFL=7.681毫米;HFOV=40.842度;TTL=9.418毫米;Fno=1.696;ImgH=6.033毫米。特別是:1.本實施例的系統長度TTL比第一實施例的系統長度TTL短;2.本實施例的縱向球差小於第一實施例的縱向球差;3.本實施例弧矢方向的場曲像差小於第一實施例弧矢方向的場曲像差;4.本實施例子午方向的場曲像差小於第一實施例子午方向的場曲像差;5.本實施例的畸變像差優於第一實施例的畸變像差。。 The detailed optical data of the fourth embodiment is shown in FIG. 26 , and the aspheric data is shown in FIG. 27 . In this embodiment, EFL=7.681 mm; HFOV=40.842 degrees; TTL=9.418 mm; Fno=1.696; ImgH=6.033 mm. In particular: 1. The system length TTL of this embodiment is shorter than that of the first embodiment; 2. The longitudinal spherical aberration of this embodiment is smaller than that of the first embodiment; 3. The sagittal direction of this embodiment The field curvature aberration of the first embodiment is smaller than the field curvature aberration of the sagittal direction; 4. The field curvature aberration of the present embodiment is smaller than the field curvature aberration of the meridian direction of the first embodiment; 5. The field curvature aberration of the present embodiment Distortion aberration is superior to that of the first embodiment. .
第五實施例 fifth embodiment
請參閱圖14,例示本發明光學成像鏡頭1的第五實施例。第五實施例在成像面4上的縱向球差請參考圖15A、弧矢方向的場曲像差請參考圖15B、子午方向的場曲像差請參考圖15C、畸變像差請參考圖15D。第五實施例之設計與第一實施例類似,不同之處在於,透鏡屈光率、透鏡曲率半徑、透鏡厚度、透鏡非球面係數或是後焦距等相關參數有別。此外,本實施例中,第三透鏡30的物側面31的光軸區域33為凸面,第四透鏡40的物側面41的光軸區域43為凸面,第五透鏡50具有負屈光率,第六透鏡60具有正屈光率,第六透鏡60的物側面61的
光軸區域63為凸面,第七透鏡70的物側面71的光軸區域73為凹面,第八透鏡80具有正屈光率,第八透鏡80的物側面81的圓周區域84為凹面。
Please refer to FIG. 14 , which illustrates a fifth embodiment of the
第五實施例詳細的光學數據如圖28所示,非球面數據如圖29所示,本實施例中,EFL=7.558毫米;HFOV=40.842度;TTL=9.454毫米;Fno=1.669;ImgH=6.118毫米。特別是:1.本實施例的系統長度TTL比第一實施例的系統長度TTL短;2.本實施例的縱向球差小於第一實施例的縱向球差;3.本實施例弧矢方向的場曲像差小於第一實施例弧矢方向的場曲像差;4.本實施例子午方向的場曲像差小於第一實施例子午方向的場曲像差;5.本實施例的畸變像差優於第一實施例的畸變像差。 The detailed optical data of the fifth embodiment is shown in Figure 28, and the aspheric data is shown in Figure 29. In this embodiment, EFL=7.558 mm; HFOV=40.842 degrees; TTL=9.454 mm; Fno=1.669; ImgH=6.118 mm. In particular: 1. The system length TTL of this embodiment is shorter than that of the first embodiment; 2. The longitudinal spherical aberration of this embodiment is smaller than that of the first embodiment; 3. The sagittal direction of this embodiment The field curvature aberration of the first embodiment is smaller than the field curvature aberration of the sagittal direction; 4. The field curvature aberration of the present embodiment is smaller than the field curvature aberration of the meridian direction of the first embodiment; 5. The field curvature aberration of the present embodiment Distortion aberration is superior to that of the first embodiment.
第六實施例 Sixth embodiment
請參閱圖16,例示本發明光學成像鏡頭1的第六實施例。第六實施例在成像面4上的縱向球差請參考圖17A、弧矢方向的場曲像差請參考圖17B、子午方向的場曲像差請參考圖17C、畸變像差請參考圖17D。第六實施例之設計與第一實施例類似,不同之處在於,透鏡屈光率、透鏡曲率半徑、透鏡厚度、透鏡非球面係數或是後焦距等相關參數有別。此外,本實施例中,第二透鏡20具有正屈光率,第三透鏡30的物側面31的光軸區域33為凸面,第四透鏡40的物側面41的光軸區域43為凸面,第五透鏡50具有負屈光率,第六透鏡60具有正屈光率,第六透鏡60的物側面61的光軸區域63為凸面,第七透鏡70的物側面71的光軸區域73為凹面。
Please refer to FIG. 16 , which illustrates a sixth embodiment of the
第六實施例詳細的光學數據如圖30所示,非球面數據如圖31所示,本實施例中,EFL=7.134毫米;HFOV=40.842度;TTL=9.183毫米;Fno=1.575; ImgH=5.937毫米。特別是:1.本實施例的系統長度TTL比第一實施例的系統長度TTL短;2.本實施例的縱向球差小於第一實施例的縱向球差;3.本實施例弧矢方向的場曲像差小於第一實施例弧矢方向的場曲像差;4.本實施例子午方向的場曲像差小於第一實施例子午方向的場曲像差;5.本實施例的畸變像差優於第一實施例的畸變像差。 The detailed optical data of the sixth embodiment is shown in Figure 30, and the aspheric data is shown in Figure 31. In this embodiment, EFL=7.134 mm; HFOV=40.842 degrees; TTL=9.183 mm; Fno=1.575; ImgH = 5.937 mm. In particular: 1. The system length TTL of this embodiment is shorter than that of the first embodiment; 2. The longitudinal spherical aberration of this embodiment is smaller than that of the first embodiment; 3. The sagittal direction of this embodiment The field curvature aberration of the first embodiment is smaller than the field curvature aberration of the sagittal direction; 4. The field curvature aberration of the present embodiment is smaller than the field curvature aberration of the meridian direction of the first embodiment; 5. The field curvature aberration of the present embodiment Distortion aberration is superior to that of the first embodiment.
第七實施例 Seventh embodiment
請參閱圖18,例示本發明光學成像鏡頭1的第七實施例。第七實施例在成像面4上的縱向球差請參考圖19A、弧矢方向的場曲像差請參考圖19B、子午方向的場曲像差請參考圖19C、畸變像差請參考圖19D。第七實施例之設計與第一實施例類似,不同之處在於,透鏡屈光率、透鏡曲率半徑、透鏡厚度、透鏡非球面係數或是後焦距等相關參數有別。此外,本實施例中,第三透鏡30具有正屈光率,第三透鏡30的物側面31的光軸區域33為凸面,第三透鏡30的像側面32的圓周區域37為凹面,第四透鏡40具有負屈光率,第五透鏡50具有負屈光率,第六透鏡60具有正屈光率,第六透鏡60的物側面61的光軸區域63為凸面,第八透鏡80的物側面81的圓周區域84為凹面。
Please refer to FIG. 18 , which illustrates a seventh embodiment of the
第七實施例詳細的光學數據如圖32所示,非球面數據如圖33所示,本實施例中:EFL=7.033毫米;HFOV=40.842度;TTL=9.103毫米;Fno=1.553;ImgH=6.049毫米。特別是:1.本實施例的系統長度TTL比第一實施例的系統長度TTL短;2.本實施例的縱向球差小於第一實施例的縱向球差;3.本實施例的畸變像差優於第一實施例的畸變像差。 The detailed optical data of the seventh embodiment are shown in Figure 32, and the aspheric data are shown in Figure 33. In this embodiment: EFL=7.033 mm; HFOV=40.842 degrees; TTL=9.103 mm; Fno=1.553; ImgH=6.049 mm. In particular: 1. The system length TTL of this embodiment is shorter than that of the first embodiment; 2. The longitudinal spherical aberration of this embodiment is smaller than that of the first embodiment; 3. The distorted image of this embodiment The difference is better than the distortion aberration of the first embodiment.
另外,各實施例之重要參數則整理於圖34與圖35中。 In addition, the important parameters of each embodiment are organized in FIG. 34 and FIG. 35 .
本發明各實施例,滿足以下透鏡面形的凹凸設計可有效降低場曲及畸變率,具有優化光學成像鏡頭系統的成像品質的特徵,以及可以達成的對應功效: In each embodiment of the present invention, the concavo-convex design that satisfies the following lens surface shapes can effectively reduce field curvature and distortion rate, have the characteristics of optimizing the imaging quality of the optical imaging lens system, and can achieve corresponding effects:
1.本發明的光學成像鏡頭1滿足第六透鏡60的像側面62的光軸區域66為凸面、第八透鏡80的物側面81的光軸區域83為凸面、第八透鏡80的像側面82的圓周區域87為凸面與D41t51/(T3+G34)≧1.700的條件,有利於設計大光圈且大像高的鏡頭。若光學成像鏡頭1進一步滿足以下條件:第一透鏡10具有正屈光率、第一透鏡10的像側面12的圓周區域17為凹面與第三透鏡30的物側面31的圓周區域34為凹面,有利於修正內視場(0.2~0.4Field)的像差,較佳的範圍為1.700≦D41t51/(T3+G34)≦6.000。
1. The
2.本發明的光學成像鏡頭1滿足第六透鏡60的像側面62的光軸區域66為凸面、第八透鏡80的物側面81的光軸區域83為凸面、第八透鏡80的像側面82的圓周區域87為凸面與D41t51/(T3+G34)≧1.700的條件,有利於設計大光圈且大像高的鏡頭。若光學成像鏡頭1進一步滿足以下條件:第三透鏡30的物側面31的圓周區域34為凹面與第四透鏡40的物側面41的圓周區域44為凹面,有利於修正內視場(0.2~0.4Field)的像差,較佳的範圍為1.700≦D41t51/(T3+G34)≦6.000。光學成像鏡頭1進一步限制第一透鏡10具有正屈光率,有利於縮短系統長度。
2. The
3.本發明的光學成像鏡頭1滿足第六透鏡60的像側面62的光軸區域66為凸面、第八透鏡80的物側面81的光軸區域83為凸面、第八透鏡80的像側面82的圓周區域87為凸面與D41t61/(T3+G34)≧3.700的條件,有利於設計大光圈且大像高的鏡頭。若光學成像鏡頭進一步滿足以下條件:第一透鏡10具有正屈光率、
第一透鏡10的像側面12的圓周區域17為凹面、第二透鏡20具有負屈光率與第四透鏡40的像側面42的圓周區域47為凸面,有利於修正內視場(0.2~0.4Field)的像差,較佳的範圍為3.700≦D41t61/(T3+G34)≦8.000。
3. The
4.本發明的光學成像鏡頭滿足V3+V8≦100.000、V7+V8≦100.000或55.000≦V2+V6的條件,有利於提高光學成像鏡頭的MTF(調製傳遞函數)增加解析度,較佳的範圍為38.000≦V3+V8≦100.000、38.000≦V7+V8≦100.000或55.000≦V2+V6≦120.000。 4. The optical imaging lens of the present invention satisfies the conditions of V3+V8≦100.000, V7+V8≦100.000 or 55.000≦V2+V6, which is conducive to improving the MTF (modulation transfer function) of the optical imaging lens to increase the resolution, the preferred range 38.000≦V3+V8≦100.000, 38.000≦V7+V8≦100.000, or 55.000≦V2+V6≦120.000.
5.本發明的光學成像鏡頭進一步滿足以下表一所列的條件式時,有助於在提供大光圈且大像高鏡頭的前提下,使各透鏡的厚度與間隔維持一適當值,避免任一參數過大而不利於該光學成像鏡頭整體之薄型化,或是避免任一參數過小而影響組裝或是提高製造上之困難度。 5. When the optical imaging lens of the present invention further satisfies the conditional formula listed in the following table 1, it helps to make the thickness and interval of each lens maintain an appropriate value under the premise of providing a large aperture and a large image and a high lens, so as to avoid any If one parameter is too large, it is not conducive to the overall thinning of the optical imaging lens, or if any parameter is too small, it will affect the assembly or increase the difficulty of manufacturing.
本發明各實施例的各種代表波長在不同高度的離軸光線皆集中在成像點附近,由每一曲線的偏斜幅度可看出不同高度的離軸光線的成像點偏差皆獲得控制而具有良好的球差、像差、畸變抑制能力。進一步參閱成像品質數據,各種代表波長彼此間的距離亦相當接近,顯示本發明的實施例在各種狀態下對不同波長光線的集中性佳而具有優良的色散抑制能力,故透過上述可知本發明的實施例具備良好光學性能。 Off-axis rays of various representative wavelengths at different heights in various embodiments of the present invention are all concentrated near the imaging point, and it can be seen from the deviation of each curve that the deviation of the imaging point of off-axis rays at different heights is controlled and has good performance. Spherical aberration, aberration, distortion suppression ability. Further referring to the imaging quality data, the distances between various representative wavelengths are also quite close, which shows that the embodiment of the present invention has good concentration of light of different wavelengths under various conditions and has excellent dispersion suppression ability, so it can be known from the above that the present invention Examples have good optical properties.
此外,另可選擇實施例參數之任意組合關係增加鏡頭限制,以利於本發明相同架構的鏡頭設計。 In addition, any combination relationship of the parameters in the embodiment can be selected to increase the lens restriction, so as to facilitate the lens design of the same structure of the present invention.
有鑑於光學系統設計的不可預測性,在本發明的架構之下,符合上 述條件式能較佳地使本發明擴大視場角、縮短系統長度、成像品質提升,或組裝良率提升而改善先前技術的缺點,而本發明實施例透鏡採用塑膠材質更能減輕鏡頭重量及節省成本。 In view of the unpredictability of optical system design, under the framework of the present invention, the above The above conditional formula can better enable the present invention to expand the field of view, shorten the system length, improve the imaging quality, or improve the assembly yield to improve the shortcomings of the prior art, and the lens of the embodiment of the present invention is made of plastic material, which can reduce the weight of the lens and cut costs.
前述所列之示例性限定關係式,亦可任意選擇性地合併不等數量施用於本發明之實施態樣中,並不限於此。在實施本發明時,除了前述關係式之外,亦可針對單一透鏡或廣泛性地針對多個透鏡額外設計出其他更多的透鏡的凹凸曲面排列等細部結構,以加強對系統性能及/或解析度的控制。須注意的是,此些細節需在無衝突之情況之下,選擇性地合併施用於本發明之其他實施例當中。 The exemplary limiting relational expressions listed above can also be arbitrarily and selectively combined and applied in different quantities in the implementation of the present invention, and are not limited thereto. When implementing the present invention, in addition to the aforesaid relational expressions, other detailed structures such as the concave-convex surface arrangement of more lenses can be additionally designed for a single lens or broadly for multiple lenses, so as to strengthen the system performance and/or Resolution control. It should be noted that these details should be selectively combined and applied to other embodiments of the present invention under the condition of no conflict.
本發明各實施例揭露之內容包含但不限於焦距、透鏡厚度、阿貝數等光學參數,舉例而言,本發明於各實施例揭露一光學參數A及一光學參數B,其中該些光學參數所涵蓋的範圍、光學參數互相之比較關係及多個實施例涵蓋的條件式範圍的具體解釋如下: The content disclosed in each embodiment of the present invention includes but not limited to optical parameters such as focal length, lens thickness, and Abbe number. For example, the present invention discloses an optical parameter A and an optical parameter B in each embodiment, wherein these optical parameters The specific explanations of the range covered, the comparative relationship between optical parameters and the conditional range covered by multiple embodiments are as follows:
(1)光學參數所涵蓋的範圍,例如:α2≦A≦α1或β2≦B≦β1,α1為光學參數A在多個實施例中的最大值,α2為光學參數A在多個實施例中的最小值,β1為光學參數B在多個實施例中的最大值,β2為光學參數B在多個實施例中的最小值。 (1) The range covered by optical parameters, for example: α 2 ≦A≦α 1 or β 2 ≦B≦β 1 , α 1 is the maximum value of optical parameter A in multiple embodiments, and α 2 is optical parameter A The minimum value in multiple embodiments, β1 is the maximum value of the optical parameter B in multiple embodiments, and β2 is the minimum value of the optical parameter B in multiple embodiments.
(2)光學參數互相之比較關係,例如:A大於B或A小於B。 (2) The comparative relationship between optical parameters, for example: A is greater than B or A is less than B.
(3)多個實施例涵蓋的條件式範圍,具體來說,由同一實施例的複數個光學參數經過可能的運算所獲得之組合關係或比例關係,該些關係定義為E。E可為例如:A+B或A-B或A/B或A*B或(A*B)1/2,而E又滿足條件式E≦γ1或E≧γ2或γ2≦E≦γ1,γ1及γ2為同一實施例的光學參數A與光學參數B經過運算所得到的 值,且γ1為本發明多個實施例中的最大值,γ2為本發明多個實施例中的最小值。 (3) The range of conditional expressions covered by multiple embodiments, specifically, the combination or proportional relationship obtained through possible operations of a plurality of optical parameters of the same embodiment, these relationships are defined as E. E can be, for example: A+B or AB or A/B or A*B or (A*B) 1/2 , and E satisfies the conditional formula E≦γ 1 or E≧γ 2 or γ 2 ≦E≦γ 1 , γ 1 and γ 2 are the values obtained by calculating the optical parameter A and optical parameter B of the same embodiment, and γ 1 is the maximum value among multiple embodiments of the present invention, and γ 2 is the value of multiple embodiments of the present invention The minimum value in .
上述光學參數所涵蓋的範圍、光學參數互相之比較關係及該些條件式的最大值、最小值及最大值最小值以內的數值範圍皆為本發明可據以實施之特徵,且皆屬於本發明所揭露的範圍。上述僅為舉例說明,不應以此為限。 The scope covered by the above-mentioned optical parameters, the comparative relationship between the optical parameters and the numerical ranges within the maximum value, minimum value and maximum minimum value of these conditional expressions are all features that the present invention can be implemented according to, and all belong to the present invention the scope of disclosure. The above is for illustration only and should not be limited thereto.
本發明之實施例皆可實施,且可於同一實施例中擷取部分特徵組合,該特徵組合相較於先前技術而言亦能達成無法預期之本案功效,該特徵組合包括但不限於面形、屈光率及條件式等特徵之搭配。本發明實施方式之揭露為闡明本發明原則之具體實施例,應不拘限本發明於所揭示的實施例。進一步言之,實施例及其附圖僅為本發明示範之用,並不受其限囿。以上所述僅為本發明之較佳實施例,凡依本發明申請專利範圍所做之均等變化與修飾,皆應屬本發明之涵蓋範圍。 All embodiments of the present invention can be implemented, and some feature combinations can be extracted in the same embodiment. Compared with the prior art, this feature combination can also achieve unexpected effects in this case. The feature combination includes but is not limited to surface shape , Refractive index and conditional formula and other characteristics of collocation. The disclosure of the embodiments of the present invention is a specific example to illustrate the principles of the present invention, and the present invention should not be limited to the disclosed embodiments. Furthermore, the embodiments and the accompanying drawings are only for demonstration purposes of the present invention, and are not intended to be limiting thereto. The above descriptions are only preferred embodiments of the present invention, and all equivalent changes and modifications made according to the scope of the patent application of the present invention shall fall within the scope of the present invention.
1:光學成像鏡頭 1: Optical imaging lens
2:光圈 2: Aperture
3:濾光片 3: Filter
4:成像面 4: Imaging surface
A1:物側 A1: Object side
A2:像側 A2: image side
I:光軸 I: optical axis
11、21、31、41、51、61、71、81:物側面 11, 21, 31, 41, 51, 61, 71, 81: the side of the object
12、22、32、42、52、62、72、82:像側面 12, 22, 32, 42, 52, 62, 72, 82: Like the side
13、16、23、26、33、36、43、46、53、56、63、66、73、76、83、86:光軸區域 13, 16, 23, 26, 33, 36, 43, 46, 53, 56, 63, 66, 73, 76, 83, 86: optical axis area
14、17、24、27、34、37、44、47、54、57、64、67、74、77、84、87:圓周區域 14, 17, 24, 27, 34, 37, 44, 47, 54, 57, 64, 67, 74, 77, 84, 87: Circumferential area
10:第一透鏡 10: First lens
20:第二透鏡 20: second lens
30:第三透鏡 30: Third lens
40:第四透鏡 40: Fourth lens
50:第五透鏡 50: fifth lens
60:第六透鏡 60: sixth lens
70:第七透鏡 70: seventh lens
80:第八透鏡 80: eighth lens
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WO2021114233A1 (en) * | 2019-12-13 | 2021-06-17 | 诚瑞光学(常州)股份有限公司 | Photographing optical lens |
CN111751961A (en) * | 2020-07-24 | 2020-10-09 | 南昌欧菲精密光学制品有限公司 | Optical lens, image capturing module and electronic device |
CN111929857B (en) * | 2020-10-13 | 2020-12-18 | 常州市瑞泰光电有限公司 | Image pickup optical lens |
CN112327450A (en) * | 2020-10-30 | 2021-02-05 | 玉晶光电(厦门)有限公司 | Optical imaging lens |
CN113484983B (en) * | 2021-06-18 | 2023-09-05 | 江西晶超光学有限公司 | Optical system, lens module and electronic equipment |
-
2021
- 2021-12-28 CN CN202111624117.3A patent/CN114114642B/en active Active
-
2022
- 2022-01-24 TW TW111102917A patent/TWI806378B/en active
- 2022-06-09 US US17/835,978 patent/US20230204912A1/en active Pending
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TW201823793A (en) * | 2016-12-27 | 2018-07-01 | 信泰光學(深圳)有限公司 | Lens assembly |
CN113640955A (en) * | 2019-08-16 | 2021-11-12 | 康达智株式会社 | Camera lens |
CN111025556A (en) * | 2019-12-23 | 2020-04-17 | 瑞声通讯科技(常州)有限公司 | Image pickup optical lens |
CN111025587A (en) * | 2019-12-28 | 2020-04-17 | 瑞声通讯科技(常州)有限公司 | Image pickup optical lens |
TW202248713A (en) * | 2021-06-11 | 2022-12-16 | 大立光電股份有限公司 | Photographing lens system, image capturing unit and electronic device |
Also Published As
Publication number | Publication date |
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US20230204912A1 (en) | 2023-06-29 |
CN114114642A (en) | 2022-03-01 |
TW202326209A (en) | 2023-07-01 |
CN114114642B (en) | 2024-07-16 |
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